Abstract: The beamlets in a multi-beam microscopy system are aligned based on coefficients of a fitted aberration model. In particular, an illuminator for directing the beamlets towards the sample is adjusted based on the coefficients to correct the aberrations. The coefficients are obtained based on measured beamlets' positions in the sample plane.

Abstract: Methods and systems to determine positions of multiple beamlets includes performing a first scan by scanning the beamlets over a first sample region and acquiring multiple cell images; and performing a second scan by scanning the beamlets over a second sample region and acquiring multiple cell images. Each cell image corresponds to a beamlet, and at least a part of an overlapped region between the first sample region and the second sample region is scanned by multiple beamlets during both the first scan and the second scan. Position of each beamlet may then be determined based on the corresponding cell images acquired during the first scan and the second scan.

Abstract: The invention relates to system and method of inspecting a specimen with a plurality of charged particle beamlets. The method comprises the steps of providing a specimen, providing a plurality of charged particle beamlets and focusing said plurality of charged particle beamlets onto said specimen, and detecting a flux of radiation emanating from the specimen in response to said irradiation by said plurality of charged particle beamlets.

Abstract: An example multi-beam scanning electron microscope (MB-SEM) for correcting both astigmatism and linear distortion at least includes an electron source coupled to provide an electron beam, an aperture plate comprising an array of apertures, the aperture plate arranged to form an array of electron beamlets from the electron beam, and an electron column including a plurality of lenses and first and second stigmators, the electron column coupled to direct the array of electron beamlets toward a sample, wherein the first and second stigmators are arranged and excited to correct both astigmatism and linear distortion.

Abstract: The invention relates to system and method of inspecting a specimen with a plurality of charged particle beamlets. The method comprises the steps of providing a specimen, providing a plurality of charged particle beamlets and focusing said plurality of charged particle beamlets onto said specimen, and detecting a flux of radiation emanating from the specimen in response to said irradiation by said plurality of charged particle beamlets.

Abstract: An electron microscope comprising: A specimen holder, for holding a specimen; An electron beam column, for producing an array of electron beams and concurrently irradiating an array of target areas of said specimen therewith; A scanning assembly, for producing relative scanning motion of said beam array with respect to the specimen; A detector, for detecting radiation emanating from the specimen in response to said irradiation, wherein said detector is: A backscattered electron detector that can be disposed proximal to the specimen at a side thereof facing said electron beam column; Provided with an array of apertures that allow passage of said electron beams from said column to the specimen; Provided with a functionally sub-divided detection surface that enables segregated detection of a backscattered electron flux produced by each individual beam.

Abstract: The invention relates to a charged particle beam device for inspection of a specimen with a plurality of charged particle beamlets. The charged particle beam device comprises a specimen holder for holding a specimen, a source for producing a beam of charged particles, and an illuminator for converting said beam of charged particles into a plurality of charged particle beamlets and focusing said plurality of charged particle beamlets onto said specimen. Furthermore, a detector assembly for detecting a flux of radiation emanating from the specimen in response to said irradiation by said plurality of charged particle beamlets is provided. As defined herein, the charged particle beam device is arranged for directing said plurality of charged particle beamlets onto said specimen in an essentially 1D pattern, wherein said essentially 1D pattern forms part of an edge of an essentially 2D geometric shape.

Abstract: A charged particle imaging apparatus comprising: A specimen holder, for holding a specimen; A particle-optical column, for: Producing a plurality of charged particle beams, by directing a progenitor charged particle beam onto an aperture plate having a corresponding plurality of apertures within a footprint of the progenitor beam; Directing said beams toward said specimen, wherein: Said aperture plate comprises a plurality of different zones, which comprise mutually different aperture patterns, arranged within said progenitor beam footprint; The particle-optical column comprises a selector device, located downstream of said aperture plate, for selecting a beam array from a chosen one of said zones to be directed onto the specimen.

Abstract: The invention relates to a method 3D defect characterization of crystalline samples in a scanning type electron microscope. The method comprises Irradiating a sample provided on a stage, selecting one set of crystal lattice planes of the sample and orienting said set to a first Bragg condition with respect to a primary electron beam impinging on said sample, and obtaining Electron Channeling Contrast Image for an area of interest on the sample. The method is characterized by performing, at least once, the steps of orienting said selected set of crystal lattice planes to a further Bragg condition by at least tilting the sample stage with the sample by a user-selected angle about a first tilt axis, and obtaining by Electron Channeling Contrast Image for a further area of interest.

Abstract: The invention relates to a method 3D defect characterization of crystalline samples in a scanning type electron microscope. The method comprises Irradiating a sample provided on a stage, selecting one set of crystal lattice planes of the sample and orienting said set to a first Bragg condition with respect to a primary electron beam impinging on said sample, and obtaining Electron Channeling Contrast Image for an area of interest on the sample. The method is characterized by performing, at least once, the steps of orienting said selected set of crystal lattice planes to a further Bragg condition by at least tilting the sample stage with the sample by a user-selected angle about a first tilt axis, and obtaining by Electron Channeling Contrast Image for a further area of interest.

Abstract: A charged particle imaging apparatus comprising: A specimen holder, for holding a specimen; A particle-optical column, for: Producing a plurality of charged particle beams, by directing a progenitor charged particle beam onto an aperture plate having a corresponding plurality of apertures within a footprint of the progenitor beam; Directing said beams toward said specimen, wherein: Said aperture plate comprises a plurality of different zones, which comprise mutually different aperture patterns, arranged within said progenitor beam footprint; The particle-optical column comprises a selector device, located downstream of said aperture plate, for selecting a beam array from a chosen one of said zones to be directed onto the specimen.

Abstract: An electron microscope comprising: A specimen holder, for holding a specimen; An electron beam column, for producing an array of electron beams and concurrently irradiating an array of target areas of said specimen therewith; A scanning assembly, for producing relative scanning motion of said beam array with respect to the specimen; A detector, for detecting radiation emanating from the specimen in response to said irradiation, wherein said detector is: A backscattered electron detector that can be disposed proximal to the specimen at a side thereof facing said electron beam column; Provided with an array of apertures that allow passage of said electron beams from said column to the specimen; Provided with a functionally sub-divided detection surface that enables segregated detection of a backscattered electron flux produced by each individual beam.

Abstract: A charged-particle microscope having a vacuum chamber comprises a specimen holder, a particle-optical column, a detector and an exchangeable column extending element. The specimen holder is for holding a specimen. The particle-optical column is for producing and directing a beam of charged particles along an axis so as to irradiate the specimen. The column has a terminal pole piece at an extremity facing the specimen holder. The detector is for detecting a flux of radiation emanating from the specimen in response to irradiation by the beam. The exchangeable column extending element is magnetically mounted on the pole piece in a space between the pole piece and the specimen holder. Methods of using the microscope are also disclosed.

Abstract: A method of producing a corrected beam of charged particles for use in a charged-particle microscope, comprising the following steps: Providing a non-monoenergetic input beam of charged particles; Passing said input beam through an optical module comprising a series arrangement of: A stigmator, thereby producing an astigmatism-compensated, energy-dispersed intermediate beam with a particular monoenergetic line focus direction; A beam selector, comprising a slit that is rotationally oriented so as to match a direction of the slit to said line focus direction, thereby producing an output beam comprising an energy-discriminated portion of said intermediate beam.

Abstract: A method of producing a corrected beam of charged particles for use in a charged-particle microscope, comprising the following steps: Providing a non-monoenergetic input beam of charged particles; Passing said input beam through an optical module comprising a series arrangement of: A stigmator, thereby producing an astigmatism-compensated, energy-dispersed intermediate beam with a particular monoenergetic line focus direction; A beam selector, comprising a slit that is rotationally oriented so as to match a direction of the slit to said line focus direction, thereby producing an output beam comprising an energy-discriminated portion of said intermediate beam.

Abstract: The invention relates to an in-column back-scattered electron detector, the detector placed in a combined electrostatic/magnetic objective lens for a SEM. The detector is formed as a charged particle sensitive surface, preferably a scintillator disk that acts as one of the electrode faces forming the electrostatic focusing field. The photons generated in the scintillator are detected by a photon detector, such as a photo-diode or a multi-pixel photon detector. The objective lens may be equipped with another electron detector for detecting secondary electrons that are kept closer to the axis. A light guide may be used to offer electrical insulation between the photon detector and the scintillator.

Abstract: The invention relates to a dual beam apparatus equipped with an ion beam column and an electron beam column having an electrostatic immersion lens. When tilting the sample, the electrostatic immersion field is distorted and the symmetry round the electron optical axis is lost. As a consequence tilting introduces detrimental effects such as traverse chromatic aberration and beam displacement. Also in-column detectors, detecting either secondary electrons or backscattered electrons in the non-tilted position of the sample, will, due to the loss of the symmetry of the immersion field, show a mix of these electrons when tilting the sample. The invention shows how, by biasing the stage with respect to the grounded electrodes closest to the sample, these disadvantages are eliminated, or at least reduced.

Abstract: The invention relates to a dual beam apparatus equipped with an ion beam column and an electron beam column having an electrostatic immersion lens. When tilting the sample, the electrostatic immersion field is distorted and the symmetry round the electron optical axis is lost. As a consequence tilting introduces detrimental effects such as traverse chromatic aberration and beam displacement. Also in-column detectors, detecting either secondary electrons or backscattered electrons in the non-tilted position of the sample, will, due to the loss of the symmetry of the immersion field, show a mix of these electrons when tilting the sample. The invention shows how, by biasing the stage with respect to the grounded electrodes closest to the sample, these disadvantages are eliminated, or at least reduced.

Abstract: The invention relates to an in-column back-scattered electron detector, the detector placed in a combined electrostatic/magnetic objective lens for a SEM. The detector is formed as a charged particle sensitive surface, preferably a scintillator disk that acts as one of the electrode faces forming the electrostatic focusing field. The photons generated in the scintillator are detected by a photon detector, such as a photo-diode or a multi-pixel photon detector. The objective lens may be equipped with another electron detector for detecting secondary electrons that are kept closer to the axis. A light guide may be used to offer electrical insulation between the photon detector and the scintillator.

Abstract: The invention relates to an in-column back-scattered electron detector, the detector placed in a combined electrostatic/magnetic objective lens for a SEM. The detector is formed as a charged particle sensitive surface, preferably a scintillator disk that acts as one of the electrode faces forming the electrostatic focusing field. The photons generated in the scintillator are detected by a photon detector, such as a photo-diode or a multi-pixel photon detector. The objective lens may be equipped with another electron detector for detecting secondary electrons that are kept closer to the axis. A light guide may be used to offer electrical insulation between the photon detector and the scintillator.